{"record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.revision/1","content_sha256":"8f69be4be3912a7e28e9693334218cc3800bbb672c3a24d6fd1b0e0442c29e28","created":"2026-10-03T07:18:00Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":["5475cf5dc5b1a72283d26dc95dc6e00d7ea4e00096a7c6492e409a1816eeb011","d20e6402a4d4b3a827eef49d38095e917972b2f2651748e9b532730c8b500987"],"salt":"255c34d21a6d20e6650d898dd1a6ec02f948ba92d47b64f01ee464fda92a946f","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"revision"},"content":{"answer_type":"yes-no","assisted_by":[],"external_id":"cm.non-abelian-quantum-hall.edge-equilibration","kind":"well-posed","literature_status":"open","n":"1","parents":[{"note":"","parent_revision":"d20e6402a4d4b3a827eef49d38095e917972b2f2651748e9b532730c8b500987","relation":"special_case"}],"plain":"The measured heat flow along the $5/2$ edge might fit the anti-Pfaffian theory if some edge channels do not exchange heat over the length of the device.","posed_since":"2018","precise":"Test whether $\\kappa_{xy} = (5/2) \\kappa_0$ at $\\nu = 5/2$ arises from an anti-Pfaffian edge whose thermal equilibration length $l_{\\mathrm{eq}}$ exceeds the device edge length $L$. This scenario predicts $\\kappa_{xy}$ depends on $L/l_{\\mathrm{eq}}$ and crosses over toward $(3/2) \\kappa_0$ for $L >> l_{\\mathrm{eq}}$. An answer is $\\kappa_{xy}(L)$ over a range of $L$ spanning $l_{\\mathrm{eq}}$.","problem_ref":null,"references":"","settled_by":"Thermal Hall measurements on $5/2$ devices with edge lengths varied by an order of magnitude at fixed temperature.","status_note":"","title":"Does partial edge equilibration explain the $5/2$ thermal Hall value","topic_ref":"ef024a2f66f3667f8a1263272e91fdabf80879850538a70f33d99943574b7c2c"},"attested":{"attestation":{"batch":null,"client_id":null,"id_token_sha256":null,"kind":"platform"},"record_hash":"b3c6740110bd04f86992b5000d7cae5ba920dac84ee0fdd852250c07fe6f6aac","schema":"pubphys.attested/1"},"envelope":{"attested_hash":"28f9aaf4edbe26fab97e7d0172a3f9462efb74a9df63219bf902d6d72f9b0e42","platform_signature":{"key_id":"c6afc19b31429869751f06879c75cd64ea92654423d15b44be775bf1310a60da","sig":"yWiYRTbabMwh_Br68OWWIFlnlmXwM5kF8l-qXpZByO8W9WjXQtKjQWPAR999Yau9KK2fO2x3BmH1HFQsE3coCQ"},"schema":"pubphys.envelope/1"},"record_hash":"b3c6740110bd04f86992b5000d7cae5ba920dac84ee0fdd852250c07fe6f6aac","leaf_index":1116}